Imaging lens and imaging apparatus

ABSTRACT

An imaging lens is constituted by, in order from the object side to the image side: a negative first lens having a concave surface toward the image side; a positive second lens having a convex surface toward the image side; a negative third lens having a concave surface toward the image side; a positive biconvex fourth lens; a positive biconvex fifth lens; and a negative sixth lens having a concave surface toward the object side. Conditional Formula (1) related to the combined focal length f12 of the first lens and the second lens and the focal length f of the entire lens system is satisfied: 
       −5&lt; f 12/ f &lt;−2  (1).

CROSS REFERENCE TO RELATED APPLICATIONS

The present application claims priority under 35 U.S.C. §119 to JapanesePatent Application No. 2015-233342 filed on Nov. 30, 2015. The aboveapplication is hereby expressly incorporated by reference in itsentirety, into the present application.

BACKGROUND

The present disclosure is related to an imaging lens which can befavorably utilized in a vehicle mounted camera, a surveillance camera, acamera for a portable terminal, etc., and to an imaging apparatusequipped with this imaging lens.

Recently, vehicle mounted cameras have been being employed to assistdrivers in confirming blind spots toward the sides and the rear, toperform image recognition of the vicinity of vehicles. Meanwhile,surveillance cameras are also being widely used for the purpose ofpreventing crime, keeping records, etc. There is demand for imaginglenses for use in such cameras to have favorable performance, whilebeing of compact configurations. A lens system having six lenses may beconsidered as an imaging lens that satisfies this demand. JapanesePatent No. 2646350, Japanese Patent No. 4556382, Japanese UnexaminedPatent Publication No. H10 (1998)-111454, Japanese Unexamined PatentPublication No. 2014-10399, Japanese Patent No. 5393276, and JapanesePatent No. 5143595 disclose lens systems having six lens configurations.

SUMMARY

There is demand for imaging lenses for use in vehicle mounted camerasand surveillance cameras to have small F numbers such that these cameraswill be utilizable even during nighttime. In addition, it is desired forsuch imaging lenses to have wide angles of view and to be capable ofobtaining favorable images not only at the central portion of an imageformation region, but also through the periphery of the image formationregion.

However, it cannot be said that the F number of the lens systemdisclosed in Japanese Patent No. 2646350 is sufficiently small to beemployed in a vehicle mounted camera or a surveillance. In addition,there is a large amount of residual aberrations, and therefore highresolution cannot be obtained through the peripheral portions of theimage formation region thereof. The lens systems having six lensconfigurations disclosed in Japanese Patent No. 4556382 and JapaneseUnexamined Patent Publication No. H10 (1998)-111454 do not sufficientlycorrect chromatic aberrations and comatic aberration, and therefore highresolution cannot be obtained through the peripheral portions of theimage formation region. A further widening of the angle of view isdesired in the imaging lenses disclosed in Japanese Unexamined PatentPublication No. 2014-10399, Japanese Patent No. 5393276, and JapanesePatent No. 5143595, in order to meet recent demand.

The present disclosure has been developed in view of the foregoingcircumstances. The present disclosure provides an imaging lens having asmall F number and a wide angle of view, which is configured to becompact and is capable of obtaining images which have favorable imagequality from the center portion through the peripheral portions of animage formation region, as well as an imaging apparatus equipped withthis imaging lens.

An imaging lens of the present disclosure consists of, in order from theobject side to the image side:

a first lens having a negative refractive power and a concave surfacetoward the image side;

a second lens having a positive refractive power and a convex surfacetoward the image side;

a third lens having a negative refractive power and a concave surfacetoward the image side;

a fourth lens having a positive refractive power and is of a biconvexshape;

a fifth lens having a positive refractive power and is of a biconvexshape; and

a sixth lens having a negative refractive power and a concave surfacetoward the object side; and

Conditional Formula (1) below is satisfied:

−5<f12/f<−2  (1)

wherein f12 is the combined focal length of the first lens and thesecond lens, and f is the focal length of the entire lens system.

In the imaging lens of the present disclosure, it is more preferable forConditional Formula (1-1) below to be satisfied.

−4.7<f12/f<−2.3  (1-1)

In the imaging lens of the present disclosure, it is preferable forConditional Formula (2) below to be satisfied, and more preferable forConditional Formula (2-1) below to be satisfied.

2<|R3|/f  (2)

−300<R3/f<−2  (2-1)

wherein R3 is the radius of curvature of the surface of the second lenstoward the object side, and f is the focal length of the entire lenssystem.

In the imaging lens of the present disclosure, it is preferable forConditional Formula (3) below to be satisfied, and more preferable forConditional Formula (3-1) below to be satisfied.

−2.1<f1/f<−1.3  (3)

−2.0<f1/f<−1.4  (3-1)

wherein f1 is the focal length of the first lens, and f is the focallength of entire lens system.

In the imaging lens of the present disclosure, it is preferable forConditional Formula (4) below to be satisfied, and more preferable forConditional Formula (4-1) below to be satisfied.

−3.5<R4/f<−2.0  (4)

−3.2<R4/f<−2.2  (4-1)

wherein R4 is the radius of curvature of the surface of the second lenstoward the image side, and f is the focal length of the entire lenssystem.

In the imaging lens of the present disclosure, it is preferable forConditional Formula (5) below to be satisfied, and more preferable forConditional Formula (5-1) below to be satisfied.

0.9<f45/f<1.3  (5)

0.9<f45/f<1.2  (5-1)

wherein f45 is the combined focal length of the fourth lens and thefifth lens, and f is the focal length of the entire lens system.

In the imaging lens of the present disclosure, it is preferable forConditional Formula (5) and Conditional Formula (6) below to besatisfied simultaneously. It is more preferable for Conditional Formula(5) and Conditional Formula (6-1) below to be satisfied simultaneously.

1.5<f4/f<3.0  (6)

1.6<f4/f<2.6  (6-1)

wherein f4 is the focal length of the fourth lens, and f is the focallength of the entire lens system.

In the imaging lens of the present disclosure, it is preferable forConditional Formula (5) and Conditional Formula (7) below to besatisfied simultaneously. It is more preferable for Conditional Formula(5) and Conditional Formula (7-1) below to be satisfied simultaneously.

1.4<f5/f<2.2  (7)

1.45<f5/f<2.1  (7-1)

wherein f5 is the focal length of the fifth lens, and f is the focallength of the entire lens system.

In the imaging lens of the present disclosure, it is preferable for thematerial of at least one of the fourth lens and the fifth lens tosatisfy Conditional Formula (8) below.

dN/dT<0  (8)

wherein dN/dT is the relative temperature coefficient of the refractiveindex of the material with respect to a wavelength of 632.8 nm within atemperature range from 20° C. to 40° C.

An imaging apparatus of the present disclosure is equipped with theimaging lens of the present disclosure.

Note that the above expression “consists of” means that lenses thatpractically have no power, optical elements other than lenses such as astop, a cover glass, and filters, and mechanical components such as lensflanges, a lens barrel, an imaging element, a camera shake correctingmechanism, etc. may be included, in addition to the constituent elementslisted above.

Note that the surface shapes, the radii of curvature, and the signs ofthe refractive powers of lenses in the above lens are those which areconsidered in the paraxial region for lenses that include asphericalsurfaces. Note that the signs of the radii of curvature are positive forsurface shapes which are convex toward the object side, and negative forsurface shapes which are convex toward the image side.

According to the present disclosure, the power arrangement and the shapeof each lens are favorably set within a lens system of a six lensconfiguration, and a predetermined conditional formula is satisfied.Therefore, it is possible to provide an imaging lens having a small Fnumber and a wide angle of view, which is configured to be compact andis capable of obtaining images which have favorable image quality fromthe center portion through the peripheral portions of an image formationregion, as well as an imaging apparatus equipped with this imaging lens.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a collection of sectional diagrams that illustrate the lensconfiguration of and the paths of light beams that pass through animaging lens according to an embodiment of the present disclosure.

FIG. 2 is a cross sectional diagram that illustrates the lensconfiguration of an imaging lens according to Example 1 of the presentdisclosure.

FIG. 3 is a cross sectional diagram that illustrates the lensconfiguration of an imaging lens according to Example 2 of the presentdisclosure.

FIG. 4 is a cross sectional diagram that illustrates the lensconfiguration of an imaging lens according to Example 3 of the presentdisclosure.

FIG. 5 is a cross sectional diagram that illustrates the lensconfiguration of an imaging lens according to Example 4 of the presentdisclosure.

FIG. 6 is a cross sectional diagram that illustrates the lensconfiguration of an imaging lens according to Example 5 of the presentdisclosure.

FIG. 7 is a cross sectional diagram that illustrates the lensconfiguration of an imaging lens according to Example 6 of the presentdisclosure.

FIG. 8 is a cross sectional diagram that illustrates the lensconfiguration of an imaging lens according to Example 7 of the presentdisclosure.

FIG. 9 is a cross sectional diagram that illustrates the lensconfiguration of an imaging lens according to Example 8 of the presentdisclosure.

FIG. 10 is a cross sectional diagram that illustrates the lensconfiguration of an imaging lens according to Example 9 of the presentdisclosure.

FIG. 11 is a collection of diagrams that illustrate aberrations of theimaging lens according to Example 1, which are spherical aberration,astigmatism, distortion, and lateral chromatic aberration in this orderfrom the left side of the drawing sheet.

FIG. 12 is a collection of diagrams that illustrate aberrations of theimaging lens according to Example 2, which are spherical aberration,astigmatism, distortion, and lateral chromatic aberration in this orderfrom the left side of the drawing sheet.

FIG. 13 is a collection of diagrams that illustrate aberrations of theimaging lens according to Example 3, which are spherical aberration,astigmatism, distortion, and lateral chromatic aberration in this orderfrom the left side of the drawing sheet.

FIG. 14 is a collection of diagrams that illustrate aberrations of theimaging lens according to Example 4, which are spherical aberration,astigmatism, distortion, and lateral chromatic aberration in this orderfrom the left side of the drawing sheet.

FIG. 15 is a collection of diagrams that illustrate aberrations of theimaging lens according to Example 5, which are spherical aberration,astigmatism, distortion, and lateral chromatic aberration in this orderfrom the left side of the drawing sheet.

FIG. 16 is a collection of diagrams that illustrate aberrations of theimaging lens according to Example 6, which are spherical aberration,astigmatism, distortion, and lateral chromatic aberration in this orderfrom the left side of the drawing sheet.

FIG. 17 is a collection of diagrams that illustrate aberrations of theimaging lens according to Example 7, which are spherical aberration,astigmatism, distortion, and lateral chromatic aberration in this orderfrom the left side of the drawing sheet.

FIG. 18 is a collection of diagrams that illustrate aberrations of theimaging lens according to Example 8, which are spherical aberration,astigmatism, distortion, and lateral chromatic aberration in this orderfrom the left side of the drawing sheet.

FIG. 19 is a collection of diagrams that illustrate aberrations of theimaging lens according to Example 9, which are spherical aberration,astigmatism, distortion, and lateral chromatic aberration in this orderfrom the left side of the drawing sheet.

FIG. 20 is a collection of diagrams that illustrate transverseaberrations of the imaging lens of Example 1.

FIG. 21 is a collection of diagrams that illustrate transverseaberrations of the imaging lens of Example 2.

FIG. 22 is a collection of diagrams that illustrate transverseaberrations of the imaging lens of Example 3.

FIG. 23 is a collection of diagrams that illustrate transverseaberrations of the imaging lens of Example 4.

FIG. 24 is a collection of diagrams that illustrate transverseaberrations of the imaging lens of Example 5.

FIG. 25 is a collection of diagrams that illustrate transverseaberrations of the imaging lens of Example 6.

FIG. 26 is a collection of diagrams that illustrate transverseaberrations of the imaging lens of Example 7.

FIG. 27 is a collection of diagrams that illustrate transverseaberrations of the imaging lens of Example 8.

FIG. 28 is a collection of diagrams that illustrate transverseaberrations of the imaging lens of Example 9.

FIG. 29 is a diagram for explaining the arrangement of imagingapparatuses to be mounted on a vehicle according to an embodiment of thepresent disclosure.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

Hereinafter, embodiments of the present disclosure will be described indetail with reference to the attached drawings. FIG. 1 is a crosssectional diagram that illustrates the lens configuration of and thepaths of light beams that pass through an imaging lens 1 according to anembodiment of the present disclosure. The example of the configurationillustrated in FIG. 1 corresponds to the configuration of an imaginglens of Example 1 to be described later. In FIG. 1, the left side is theobject side, and the right side is the image side. In addition, FIG. 1also illustrates the optical paths of an axial light beam 2 and a lightbeam 3 at a maximum angle of view.

As illustrated in FIG. 1, the imaging lens 1 is constituted by sixlenses, which are, in order from the object side to the image side alongan optical axis Z, a first lens L1 having a negative refractive powerand a concave surface toward the image side; a second lens L2 having apositive refractive power and a convex surface toward the image side; athird lens L3 having a negative refractive power and a concave surfacetoward the image side; a fourth lens L4 having a positive refractivepower and is of a biconvex shape; a fifth lens L5 having a positiverefractive power and is of a biconvex shape; and a sixth lens L6 havinga negative refractive power and a concave surface toward the objectside.

Widening of the angle of view is facilitated by configuring the imaginglens such that the first lens L1, which is the lens most toward theobject side, is a negative lens. In addition, a widening of the angle ofview is also facilitated by configuring the surface of the first lens L1toward the image side to be concave. By configuring the second lens L2to be a positive lens having a convex surface toward the image side,aberrations can be corrected at various angles of view while suppressingthe generation of negative distortion. In addition, by the third lens L3through the sixth lens L6 being of the configurations described above,these four lenses form a configuration with favorable symmetry, andaberrations can be favorably and effectively corrected.

By the configurations of the first lens L1 through the sixth lens L6being those described above, the generation of distortion and lateralchromatic aberration can be suppressed even if the angle of view of alens system having a small F number is widened, for example, to an angleof view of 100 degrees or greater, and it will be possible to obtain alens system having high resolution from the central portion to theperipheral portions of an image formation region.

The imaging lens 1 is configured such that Conditional Formula (1) belowis satisfied.

−5<f12/f<−2  (1)

wherein f12 is the combined focal length of the first lens and thesecond lens, and f is the focal length of the entire lens system.

By configuring the imaging lens such that the value of f12/f is not lessthan or equal to the lower limit defined in Conditional Formula (1), thenegative refractive power of the first lens L1 can be prevented frombecoming excessively weak and will become an appropriate value.Therefore, a widening of the angle of view is facilitated. Byconfiguring the imaging lens such that the value of f12/f is not greaterthan or equal to the upper limit defined in Conditional Formula (1), thepositive refractive power of the second lens L2 can be maintained at anappropriate value. Therefore, the generation of a great amount ofnegative distortion can be prevented, while suppressing the generationof higher order aberrations. Such a configuration is advantageous fromthe viewpoint of realizing favorable optical performance from thecentral portion to the peripheral portions of an image formation region,even in a lens system having a small F number and a wide angle of view.

It is more preferable for Conditional Formula (1-1) below to besatisfied, in order to cause the advantageous effects related toConditional Formula (1) to become more prominent.

−4.7<f12/f<−2.3  (1-1)

In addition, it is preferable for Conditional Formula (2) below to besatisfied in the imaging lens 1.

2<|R3|/f  (2)

wherein R3 is the radius of curvature of the surface of the second lenstoward the object side, and f is the focal length of the entire lenssystem.

By configuring the imaging lens such that the value of |R3|/f is notless than or equal to the lower limit defined in Conditional Formula(2), the absolute value of the radius of curvature of the surface of thesecond lens L2 toward the object side can be prevented from becomingexcessively small, and the angle formed by a light ray that enters thesurface of the second lens L2 toward the object side from the objectside and a line normal to the surface at the point at which the incidentlight ray intersects with the surface can be maintained at anappropriate value. Therefore, the generation of higher order aberrationscan be suppressed, and flare components of comatic aberrations can besuppressed particularly for peripheral light beams. As a result,aberrations can be favorably corrected throughout the entirety of animage formation region.

Note that the second lens L2 may be a positive meniscus lens having aconvex surface toward the image side. In this case, the generation of agreat amount of negative distortion can be suppressed, while alsosuppressing the generation of higher order aberrations.

Further, it is preferable for Conditional Formula (2-1) below to besatisfied.

−300<R3/f<−2  (2-1)

By configuring the imaging lens such that the value of R3/f is not lessthan or equal to the lower limit defined in Conditional Formula (2-1),it will be possible to prevent the angle formed by a light ray thatenters the surface of the second lens L2 toward the object side from theobject side and a line normal to the surface at the point at which theincident light ray intersects with the surface from becoming excessivelysmall. As a result, favorable correction of distortion will becomepossible. By configuring the imaging lens such that the value of R3/f isnot greater than or equal to the upper limit defined in ConditionalFormula (2-1), the aforementioned angle can be prevented from becomingexcessively great. Therefore, the generation of higher order aberrationscan be suppressed, and flare components of comatic aberrations can besuppressed particularly for peripheral light beams. As a result,aberrations can be favorably corrected throughout the entirety of animage formation region.

In addition, it is preferable for Conditional Formula (3) below to besatisfied in the imaging lens 1.

−2.1<f1/f<−1.3  (3)

wherein f1 is the focal length of the first lens, and f is the focallength of entire lens system.

By configuring the imaging lens such that the value of f1/f is not lessthan or equal to the lower limit defined in Conditional Formula (3),negative refractive power can be prevented from becoming excessivelyweak, and therefore achieving a widening of the angle of view isfacilitated. By configuring the imaging lens such that the value of f1/fis not greater than or equal to the upper limit defined in ConditionalFormula (3), a widening of the angle of view can be achieved and thegeneration of a great amount of negative spherical aberration can beprevented. Therefore, favorable correction of aberrations will becomepossible. It is more preferable for Conditional Formula (3-1) below tobe satisfied, in order to cause the advantageous effects related toConditional Formula (3) to become more prominent.

−2.0<f1/f<−1.4  (3-1)

In addition, it is preferable for Conditional Formula (4) below to besatisfied in the imaging lens 1.

−3.5<R4/f<−2.0  (4)

wherein R4 is the radius of curvature of the surface of the second lenstoward the image side, and f is the focal length of the entire lenssystem.

Conditional Formula (4) is a conditional formula for favorablycorrecting aberrations from the third lens L3 through the sixth lens L6by refracting light rays, which are refracted in a direction away fromthe optical axis Z at the surface of the second lens L2 toward theobject side, in a direction toward the optical direction. By ConditionalFormula (4) being satisfied, the principal light rays of light beams canbe returned to the vicinity of the center of the third lens L3 withouthigher order aberrations being generated. Therefore, an aperture stop Stcan be provided at a position away from an image formation plane Sim.Thereby, light rays at various angles of view can be separated andaberrations can be corrected by lenses which are positioned at the imageside of the aperture stop St, and as a result, high imaging performancecan be obtained. It is more preferable for Conditional Formula (4-1)below to be satisfied, in order to cause the advantageous effectsrelated to Conditional Formula (4) to become more prominent.

−3.2<R4/f<−2.2  (4-1)

Note that it is preferable for the aperture stop St to be positionedbetween the surface of the second lens L2 toward the object side and thesurface of the third lens L3 toward the image side. In this case, theaforementioned correction of aberrations can be performed morefavorably. Further, the incident angles of principal light rays of offaxis light beams that enter the image formation surface Sim can besuppressed, and therefore improvements in amounts of light at peripheralportions of the image formation region become possible. FIG. 1illustrates an example in which the aperture stop St is positionedbetween the surface of the second lens L2 toward the image side and thesurface of the third lens L3 toward the object side. However, theaperture stop St illustrated in FIG. 1 does not necessarily representthe size or the shape thereof, but represents the position thereof alongthe optical axis.

In addition, it is preferable for Conditional Formula (5) below to besatisfied in the imaging lens 1.

0.9<f45/f<1.3  (5)

wherein f45 is the combined focal length of the fourth lens and thefifth lens, and f is the focal length of the entire lens system.

Conditional Formula (5) is a conditional formula for appropriatelymaintaining the combined refractive power of the fourth lens L4 and thefifth lens L5. By configuring the imaging lens such that the value off45/f is not less than or equal to the lower limit defined inConditional Formula (5), the combined refractive power can be preventedfrom becoming excessively strong, and the generation of higher orderaberrations can be suppressed. By configuring the imaging lens such thatthe value of f45/f is not greater than or equal to the upper limitdefined in Conditional Formula (5), positive refractive power can beprevented from becoming excessively weak, and negative sphericalaberration which is generated by lens groups positioned at the objectside of the fourth lens L4 can be favorably corrected. It is morepreferable for Conditional Formula (5-1) below to be satisfied, in orderto cause the advantageous effects related to Conditional Formula (5) tobecome more prominent.

0.9<f45/f<1.2  (5-1)

In addition, it is preferable for Conditional Formula (5) andConditional Formula (6) below to be satisfied simultaneously in theimaging lens 1.

1.5<f4/f<3.0  (6)

wherein f4 is the focal length of the fourth lens, and f is the focallength of the entire lens system.

Conditional Formula (6) is a conditional formula which is required forthe fourth lens L4 to favorably correct and converge negative sphericalaberration which is generated by lens groups positioned at the objectside of the fourth lens L4, in order to widen the angle of view. Byconfiguring the imaging lens such that the value of f4/f is not lessthan or equal to the lower limit defined in Conditional Formula (6),positive refractive power will be prevented from becoming excessivelystrong, and the absolute values of the radii of curvature of the lenssurfaces of the fourth lens L4 toward the object side and the image sidecan be prevented from becoming excessively small. Therefore, thegeneration of higher order aberrations can be suppressed. By configuringthe imaging lens such that the value of f4/f is not greater than orequal to the upper limit defined in Conditional Formula (6), positiverefractive power will be prevented from becoming excessively weak, andnegative spherical aberration which is generated by lens groupspositioned at the object side of the fourth lens L4 can be favorablycorrected. In addition, it is necessary for each of the fourth lens L4and the fifth lens L5 to have a certain degree of refractive power. Forthis reason, by configuring the imaging lens such that the value of f4/fis not greater than or equal to the upper limit defined in ConditionalFormula (6), the positive refractive power of the fourth lens L4 will beprevented from becoming excessively weak, the refractive power of thefifth lens L5 will be prevented from becoming excessively strong, andfavorable correction of aberrations will become possible. It is morepreferable for Conditional Formula (6-1) below to be satisfied, in orderto cause the advantageous effects related to Conditional Formula (6) tobecome more prominent.

1.6<f4/f<2.6  (6-1)

In addition, it is preferable for Conditional Formula (5) andConditional Formula (7) below to be satisfied simultaneously in theimaging lens 1.

1.4<f5/f<2.2  (7)

wherein f5 is the focal length of the fifth lens, and f is the focallength of the entire lens system.

Conditional Formula (7) is a conditional formula which is required forthe fifth lens L5 to favorably correct and converge negative sphericalaberration which is generated by lens groups positioned at the objectside of the fourth lens L4, in order to widen the angle of view. Byconfiguring the imaging lens such that the value of f5/f is not lessthan or equal to the lower limit defined in Conditional Formula (7),positive refractive power will be prevented from becoming excessivelystrong, and the absolute values of the radii of curvature of the lenssurfaces of the fifth lens L5 toward the object side and the image sidecan be prevented from becoming excessively small. Therefore, thegeneration of higher order aberrations can be suppressed. By configuringthe imaging lens such that the value of f5/f is not greater than orequal to the upper limit defined in Conditional Formula (7), positiverefractive power will be prevented from becoming excessively weak, andnegative spherical aberration which is generated by lens groupspositioned at the object side of the fourth lens L4 can be favorablycorrected. In addition, it is necessary for each of the fourth lens L4and the fifth lens L5 to have a certain degree of refractive power. Forthis reason, by configuring the imaging lens such that the value of f5/fis not greater than or equal to the upper limit defined in ConditionalFormula (7), the positive refractive power of the fifth lens L5 will beprevented from becoming excessively weak, the refractive power of thefourth lens L4 will be prevented from becoming excessively strong, andfavorable correction of aberrations will become possible. It is morepreferable for Conditional Formula (7-1) below to be satisfied, in orderto cause the advantageous effects related to Conditional Formula (7) tobecome more prominent.

1.45<f5/f<2.1  (7-1)

It is even more preferable for both of Conditional Formulae (6) and (7)to be satisfied simultaneously with Conditional Formula (5), for thereasons described above.

In addition, it is preferable for the material of at least one of thefourth lens L4 and the fifth lens L5 to satisfy Conditional Formula (8)below.

dN/dT<0  (8)

wherein dN/dT is the relative temperature coefficient of the refractiveindex of the material with respect to a wavelength of 632.8 nm within atemperature range from 20° C. to 40° C.

By employing a material that satisfies Conditional Formula (8), thefocal point position moving greatly in a direction that approaches thelens accompanying increases in temperature can be suppressed. Inaddition, the focal point position moving greatly in a direction awayfrom the lens accompanying decreases in temperature can also besuppressed. For this reason, the amount of movement of an imageformation position caused by expansion and contraction of a casing andchanges in the focal point position of the lens system accompanyingchanges in temperature can be decreased. Therefore, deterioration inresolution due to changes in temperature can be suppressed. There isdemand for imaging lenses for use in vehicle mounted cameras,surveillance cameras, cameras for portable terminals, etc. to have highweather resistance properties and to be utilizable in a wide temperaturerange from outdoors in cold weather climates to inside vehicles duringthe summer in tropical climates. Therefore, a configuration thatsatisfies Conditional Formula (8) is advantageous from this viewpoint.

In addition, the imaging lens 1 may be provided with members among thelenses that cut off a portion of peripheral light rays within a rangethat does not cause practical problems with respect to peripheralamounts of light, such as stops. Peripheral light rays are light raysthat pass through the peripheral portion of the entrance pupil of theoptical system from among light rays from an off axis object point. Byproviding a member that cuts off peripheral light rays in this manner,the image quality can be improved at the peripheral portion of the imageformation region. In addition, this member cuts off light that generatesghosts, and therefore it becomes possible to reduce the generation ofghosts. FIG. 1 illustrates an example in which a first light shieldingmember 4 and a second light shielding member 5 having circular openingscentered on the optical axis and cut off a portion of peripheral lightrays are respectively positioned between the second lens L2 and thethird lens L3 and between the third lens L3 and the fourth lens L4. Notethat the first light shielding member 4 and the second light shieldingmember 5 illustrated in FIG. 1 do not necessarily represent the sizes orshapes thereof, but their positions along the optical axis.

In addition, it is preferable for a protective multiple layer filmcoating to be administered in the case that the present imaging lens isto be utilized in extreme environments. Further, an antireflectioncoating may be administered in addition to the protective coating, inorder to reduce ghost light and the like during utilization of theimaging lens.

In addition, in the case that this imaging lens is applied to an imagingapparatus, a cover glass, prisms, and various filters, such as aninfrared cutoff filter and a low pass filter, may be provided betweenthe lens system and an image formation plane Sim, depending on theconfiguration of the imaging apparatus. Note that these filters may beprovided among the lenses instead of being provided between the lenssystem and the image formation plane Sim. As a further alternative,coatings that exhibit the same effects as these filters may beadministered on the lens surfaces of the lenses.

Arbitrary combinations of the preferred configurations and possibleconfigurations described above, including the configurations related tothe conditional formulae, are possible. It is preferable for theseconfigurations to be selectively adopted as appropriate according todesired specifications. For example, the imaging lens 1 may beconfigured to have a small F number and a wide angle of view, configuredto be compact and capable of obtaining images which have favorable imagequality from the center portion through the peripheral portion of animage formation region, by adopting the configurations described aboveas appropriate. Note that here, a small F number means that the F numberis 2.3 or less, and a wide angle of view means that the full angle ofview is 100 degrees or greater.

Next, examples of numerical values of the imaging lens of the presentdisclosure will be described.

Example 1

FIG. 2 is a cross sectional diagram that illustrates the lensconfiguration of the imaging lens of Example 1. The imaging lens ofExample 1 is constituted by six lenses, which are the first lens L1through the sixth lens L6. In FIG. 2, the left side is the object sideand the right side is the image side. FIG. 2 also illustrates anaperture stop St as well as the aforementioned first light shieldingmember 4 and the second light shielding member 5. Note that the aperturestop St, the first light shielding member 4, and the second lightshielding member 5 illustrated in FIG. 2 do not necessarily representthe sizes and shapes thereof, but only the positions thereof along theoptical axis Z.

Basic lens data are shown in Table 1, and data related to asphericalsurface coefficients are shown in Table 2 for the imaging lens ofExample 1. In Table 1, ith (i=1, 2, 3, . . . ) lens surface numbers thatsequentially increase from the object side to the image side, with thesurface toward the object side of the constituent element at the mostobject side designated as first, are shown in the column Si. The radiiof curvature of ith surfaces are shown in the column Ri. The distancesbetween an ith surface and an i+1st surface along the optical axis Z areshown in the column Di. The refractive indices with respect to the dline (wavelength: 587.6 nm) of jth (j=1, 2, 3, . . . ) constituentelements that sequentially increase from the object side to the imageside, with the constituent element at the most object side designated asfirst, are shown in the column Ndj. The Abbe's numbers with respect tothe d line of jth constituent elements are shown in the column vdj.

Here, the signs of the radii of curvature are positive in cases that thesurface shape is convex toward the object side, and negative in casesthat the surface shape is convex toward the image side. Table 1 alsoshows data regarding the aperture stop St. Text reading “(St)” isindicated along with a surface number in the column of the surfacenumber at the surface corresponding to the aperture stop. The value inthe lowermost row of column Di is the distance between the surface mosttoward the image side within the table and an image formation plane Sim.Data related to the first light shielding member 4 and the second lightshielding member 5 are summarized with those of the other Examples asshown in Table 19.

The values of the focal length f of the entire lens system, the backfocus Bf as an air converted length, the F number F No., and the fullangle of view 2ω with reference to the d line are shown above the frameof Table 1.

In Table 1, the surface numbers of aspherical surfaces are appended withthe mark “*”, and numerical values that represent paraxial radii ofcurvature are shown as the radii of curvature of the asphericalsurfaces. Table 2 shows aspherical surface coefficients related to theseaspherical surfaces. The aspherical surface coefficients are the valuesof the coefficients KA and Am (m=4, 6, 8, 10, 12, 14) in the asphericalsurface formula below.

${Zd} = {\frac{C \times h^{2}}{1 + \sqrt{1 - {{KA} \times C^{2} \times h^{2}}}} + {\sum\limits_{m}{{Am} \times h^{m}}}}$

wherein Zd is the depth of the aspherical surface (the length of anormal line that extends from a point on the aspherical surface at aheight h to a plane perpendicular to the optical axis that contacts theapex of the aspherical surface), h is the height (the distance from theoptical axis), C is the paraxial curvature, and KA and Am are asphericalsurface coefficients (m=4, 6, 8, 10, 12, 14).

In the data shown in each of the tables below, degrees are used as theunits for angles and mm are used as the units for lengths. However, itis possible for optical systems to be proportionately enlarged orproportionately reduced and utilized. Therefore, other appropriate unitsmay be used. In addition, numerical values which are rounded off at apredetermined number of digits are shown in each of the tables below.

TABLE 1 Example 1 f = 3.36, Bf = 3.92, F No. = 2.28, 2ω = 121.8° Si RiDi Ndj νdj *1 46.3782 1.0099 1.58313 59.38 *2 3.3919 2.4498 *3 −11.87212.4923 1.80610 40.93 *4 −7.8254 1.6399 5 (St) ∞ 0.5168 6 22.0925 0.79991.92286 18.90 7 10.4213 1.5098 *8 11.4513 2.0399 1.80610 40.93 *9−7.5199 0.1551 *10 9.5049 3.1808 1.61881 63.85 *11 −4.7573 0.2499 12−4.2346 0.7999 1.92286 18.90 13 −28.6463 3.9229

TABLE 2 Example 1 Surface Number 1 2 3 4 KA  1.0256714E+00 9.8030967E−01  4.9823534E+00 −2.9119851E+00  A4 −5.8067886E−05−2.8193943E−04 −2.4551451E−05 −1.3518732E−04  A6  1.7109404E−06 2.1941078E−05 −1.4720654E−04 3.5092421E−05 A8  8.6387002E−08−2.6438429E−06  3.3454386E−05 7.3383896E−06 A10  3.0651735E−10−1.0321548E−06 −2.5251731E−06 −1.9981789E−06  A12 −3.8902319E−11−2.4352323E−08 −8.2938235E−08 1.7803953E−07 A14 −2.2571402E−12 6.5133835E−09  2.4689797E−08 2.2661663E−08 Surface Number 8 9 10 11 KA−2.3407927E+00 −6.6734789E−02  4.1008059E−01 9.6949840E−01 A4 3.4747350E−04 −1.0415036E−04 −4.2442346E−05 1.7917967E−05 A6−9.7158216E−05 −5.3441524E−05 −4.4486444E−06 1.3296517E−05 A8−2.7989415E−06  1.0659431E−07  7.9941785E−07 6.4552362E−07 A10−8.8763973E−07 −8.1479409E−07  2.9678085E−08 −3.3943306E−08  A12−8.0268334E−08 −1.6493278E−09  3.0389364E−08 5.4481103E−09 A14−6.2337163E−09  2.1371982E−09 −4.7342740E−09 −3.4611587E−09 

FIG. 11 and FIG. 20 are collections of diagrams that illustrate variousaberrations of the imaging lens of Example 1 in a state focused on anobject at infinity. In FIG. 11, diagrams that illustrate sphericalaberration, astigmatism, distortion, and lateral chromatic aberrationare illustrated in this order from the left side of the drawing sheet.The diagram that illustrates spherical aberration shows aberrationsrelated to the d line (wavelength: 587.6 nm), the C line (wavelength:656.3 nm), and the F line (wavelength: 486.1 nm), as a solid line, along broken line, and a dotted line, respectively. In the diagram thatillustrates astigmatism, aberrations in the sagittal direction andaberrations in the tangential direction related to the d line areindicated by a solid line and a dotted line, respectively. In thediagram that illustrates distortion, aberrations related to the d lineare shown by a solid line. In the diagram that illustrates lateralchromatic diagram, aberrations related to the C line and the F line areshown as a long broken line and a dotted line, respectively. In thediagram that illustrates spherical aberration, “FNo.” denotes the Fnumber. In the other diagrams that illustrate the aberrations, ω denoteshalf angles of view.

FIG. 20 is a collection of diagrams that illustrate transverseaberrations with respect to half angles of view co in the tangentialdirection at the left side of the drawing sheet, and transverseaberrations with respect to half angles of view C in the sagittaldirection at the right side of the drawing sheet. These diagramsillustrate transverse aberration related to the d line. Note that theaberration diagrams of FIG. 11 and FIG. 20 are for a state in which thefirst light shielding member 4 and the second light shielding member 5are provided as shown in Table 19.

The symbols, the meanings, and the manners in which the various piecesof data are described in the description of Example 1 above are the samefor the examples to be described below unless otherwise noted.Therefore, redundant descriptions will be omitted hereinafter.

Example 2

FIG. 3 is a cross sectional diagram that illustrates the lensconfiguration of the imaging lens of Example 2. Basic lens data areshown in Table 3 and aspherical surface coefficients are shown in Table4 for the imaging lens of Example 2. In addition, FIG. 12 and FIG. 21are collections of diagrams that illustrate various aberrations of theimaging lens of Example 2 in a state focused on an object at infinity.

TABLE 3 Example 2 f = 3.35, Bf = 4.30, F No. = 2.27, 2ω = 122.6° Si RiDi Ndj νdj *1 46.3783 1.0112 1.58313 59.38 *2 3.1881 2.5131 *3 −13.44652.5001 1.80610 40.93 *4 −8.0867 1.6700 5 (St) ∞ 0.2499 6 63.9530 0.86321.92286 18.90 7 15.0562 1.6101 *8 10.5055 2.0399 1.80610 40.93 *9−7.6909 0.1549 *10 10.4629 2.8474 1.61881 63.85 *11 −4.9605 0.2699 12−4.2728 0.8000 1.92286 18.90 13 −25.9702 4.3020

TABLE 4 Example 2 Surface Number 1 2 3 4 KA  1.0015654E+00 9.8034752E−01  4.9874050E+00 −2.9118623E+00  A4 −5.8089014E−05−2.8201766E−04 −2.4589817E−05 −1.3639095E−04  A6  1.7351094E−06 2.3925431E−05 −1.4718131E−04 3.5103502E−05 A8  5.0519007E−08−2.6455255E−06  3.3461694E−05 7.6640931E−06 A10  3.2883104E−10−9.3781604E−07 −2.5125247E−06 −2.0643524E−06  A12 −4.0227881E−11−2.4352323E−08 −2.1118172E−07 −1.5804988E−08  A14 −2.2293092E−12 4.7205806E−09  4.6863149E−08 7.0019599E−08 Surface Number 8 9 10 11 KA−2.3378548E+00 −6.5770611E−02  4.0941414E−01 9.7069922E−01 A4 3.4548187E−04 −1.0411375E−04 −4.2403539E−05 1.7967529E−05 A6−9.7186039E−05 −5.3459088E−05 −4.4562616E−06 1.3278971E−05 A8−3.0722073E−06  1.0501901E−07  7.9299463E−07 6.4335672E−07 A10−1.7446341E−06 −8.1956928E−07  3.3983273E−08 −4.4569123E−08  A12 3.2937745E−07 −3.2259681E−08  4.1915724E−08 2.3208298E−08 A14−5.3243745E−08 −1.3452632E−09 −7.9359766E−09 −7.7610359E−09 

Example 3

FIG. 4 is a cross sectional diagram that illustrates the lensconfiguration of the imaging lens of Example 3. Basic lens data areshown in Table 5 and aspherical surface coefficients are shown in Table6 for the imaging lens of Example 3. In addition, FIG. 13 and FIG. 22are collections of diagrams that illustrate various aberrations of theimaging lens of Example 3 in a state focused on an object at infinity.

TABLE 5 Example 3 f = 3.31, Bf = 4.12, F No. = 2.26, 2ω = 130.0° Si RiDi Ndj νdj 1 46.3786 1.0200 1.58313 59.38 2 3.2332 2.5830 *3 −16.20661.8749 1.80610 40.93 *4 −9.4864 1.7610 5 (St) ∞ 0.2500 6 212.1128 0.85671.95906 17.47 7 20.7117 2.0115 *8 9.4219 2.0465 1.80610 40.93 *9 −9.14760.1549 10 9.2275 3.1492 1.61881 63.85 11 −5.0420 0.2840 12 −4.12260.7999 1.95906 17.47 13 −17.3321 4.1164

TABLE 6 Example 3 Surface Number 3 4 8 9 KA  4.9943054E+00−3.2075243E+00  −2.8591645E+00 −5.9096017E−02 A4 −3.4305098E−04−1.6248734E−04   3.0021340E−04 −1.0139010E−04 A6 −9.8793083E−05−1.0979007E−05  −9.0667963E−05 −6.0973192E−05 A8  3.4851534E−057.7385234E−06 −1.1500681E−06 −1.7379319E−07 A10 −2.9967738E−061.4849994E−07  3.8849226E−07 −7.6958361E−07 A12 −4.5125120E−081.4258051E−08 −6.1071120E−08 −1.1377396E−08 A14  1.8338019E−087.2166943E−09 −8.3794403E−08 −1.5655533E−08

Example 4

FIG. 5 is a cross sectional diagram that illustrates the lensconfiguration of the imaging lens of Example 4. Basic lens data areshown in Table 7 and aspherical surface coefficients are shown in Table8 for the imaging lens of Example 4. In addition, FIG. 14 and FIG. 23are collections of diagrams that illustrate various aberrations of theimaging lens of Example 4 in a state focused on an object at infinity.

TABLE 7 Example 4 f = 3.38, Bf = 4.27, F No. = 2.29, 2ω = 125.4° Si RiDi Ndj νdj 1 46.3782 1.0201 1.77198 49.64 2 3.4707 2.4399 *3 −891.98621.8921 1.80610 40.93 *4 −10.1687 2.2620 5 (St) ∞ 0.2501 6 11.9890 0.80001.85000 22.84 7 7.7518 2.0614 *8 16.6100 2.0630 1.80610 40.93 *9 −9.33480.1549 10 7.7060 3.1235 1.70788 54.61 11 −5.8063 0.2700 12 −4.86990.8000 1.95906 17.47 13 −39.2316 4.2683

TABLE 8 Example 4 Surface Number 3 4 8 9 KA 5.0000090E+00 8.5019836E−01−2.7418395E+00 −1.7492582E−01 A4 −2.0050681E−04  −1.8499323E−04  3.0297894E−04 −8.7593446E−05 A6 −1.1390021E−04  2.7187491E−05−1.0507689E−04 −6.1083751E−05 A8 3.7236185E−05 7.8688595E−06 2.7014417E−07  6.3442454E−07 A10 −2.8017799E−06  −8.1502255E−07  3.9331389E−07 −8.2423003E−07 A12 6.8811735E−09 −3.6155519E−08 −4.3585420E−07 −8.3853579E−09 A14 7.1620841E−09 4.6971967E−09−5.5369866E−09 −2.0161176E−09

FIG. 6 is a cross sectional diagram that illustrates the lensconfiguration of the imaging lens of Example 5. Basic lens data areshown in Table 9 and aspherical surface coefficients are shown in Table10 for the imaging lens of Example 5. In addition, FIG. 15 and FIG. 24are collections of diagrams that illustrate various aberrations of theimaging lens of Example 5 in a state focused on an object at infinity.

TABLE 9 Example 5 f = 3.34, Bf = 4.51, F No. = 2.27, 2ω = 124.6° Si RiDi Ndj νdj 1 37.3673 1.0199 1.69350 53.20 2 3.1247 2.1266 *3 −19.77271.9732 1.80610 40.93 *4 −9.0515 1.6799 5 (St) ∞ 0.2524 6 45.3710 0.94871.84666 23.78 7 12.3515 1.7098 *8 12.9401 2.0401 1.80610 40.93 *9−7.7675 0.1549 10 8.4761 3.3422 1.61881 63.85 11 −5.0533 0.2997 12−4.2261 0.7999 1.95906 17.47 13 −17.0894 4.5100

TABLE 10 Example 5 Surface Number 3 4 8 9 KA  4.9934146E+00−2.5862638E+00 −2.8404148E+00 −1.1058901E−01 A4 −2.0111170E−04−1.8820563E−04  3.0012683E−04 −9.2440788E−05 A6 −1.1266814E−04 3.1690949E−05 −9.0452106E−05 −6.1338505E−05 A8  3.4345220E−05 8.8245332E−06 −1.0920471E−06 −2.0351419E−07 A10 −2.4796008E−06−6.8754544E−07 −1.2564167E−06 −7.6947124E−07 A12 −1.2073443E−07−3.3955914E−07 −7.9045891E−08 −1.7485420E−08 A14  3.7833736E−08 1.0008518E−07 −5.6169679E−08 −9.8143615E−09

Example 6

FIG. 7 is a cross sectional diagram that illustrates the lensconfiguration of the imaging lens of Example 6. Basic lens data areshown in Table 11 and aspherical surface coefficients are shown in Table12 for the imaging lens of Example 6. In addition, FIG. 16 and FIG. 25are collections of diagrams that illustrate various aberrations of theimaging lens of Example 6 in a state focused on an object at infinity.

TABLE 11 Example 6 f = 3.33, Bf = 3.13, F No. = 2.28, 2ω = 123.0° Si RiDi Ndj νdj *1 46.3777 1.0100 1.58313 59.38 *2 3.3214 2.4470 *3 −14.60021.9000 1.80610 40.93 *4 −9.7900 1.5900 5 (St) ∞ 0.2500 6 10.6791 0.80001.92286 18.90 7 7.4590 2.3180 *8 8.5434 2.4120 1.65160 58.55 *9 −6.92840.1550 *10 6.7792 3.4530 1.49700 81.54 *11 −5.3799 0.5720 12 −4.22400.8000 1.92286 18.90 13 −20.4123 3.1282

TABLE 12 Example 6 Surface Number 1 2 3 4 KA  1.0388813E+00 9.8027916E−01  4.9920557E+00 −2.9130832E+00  A4 −5.8026923E−05−2.8184824E−04 −2.4637941E−05 −1.3499903E−04  A6  1.6829806E−06 2.1929698E−05 −1.4719627E−04 3.5082499E−05 A8  1.1247450E−07−2.8553381E−06  3.3460159E−05 7.4142118E−06 A10  1.8703198E−10−1.0399483E−06 −2.5241465E−06 −2.4316303E−06  A12 −3.8167564E−11−2.4352323E−08 −7.1887757E−08 2.3743904E−07 A14 −2.2944987E−12 1.3279288E−08  2.3973346E−08 2.1016750E−08 Surface Number 8 9 10 11 KA−2.4001174E+00 −6.6650853E−02  4.1114783E−01 9.6810255E−01 A4 3.4410756E−04 −1.0417861E−04 −4.2394618E−05 1.7903684E−05 A6−9.7140471E−05 −5.3433764E−05 −4.4436767E−06 1.3280146E−05 A8−3.0047668E−06  1.1527252E−07  8.0670541E−07 6.5988611E−07 A10−1.9130765E−06 −7.9849999E−07  1.2824150E−08 −4.0629926E−08  A12 3.5028996E−07  6.3559364E−09  5.0995653E−10 8.3273147E−09 A14−6.0558079E−08 −6.9329469E−09 −5.2398882E−09 −6.6713943E−09 

Example 7

FIG. 8 is a cross sectional diagram that illustrates the lensconfiguration of the imaging lens of Example 7. Basic lens data areshown in Table 13 and aspherical surface coefficients are shown in Table14 for the imaging lens of Example 7. In addition, FIG. 17 and FIG. 26are collections of diagrams that illustrate various aberrations of theimaging lens of Example 7 in a state focused on an object at infinity.

TABLE 13 Example 7 f = 3.31, Bf = 2.92, F No. = 2.28, 2ω = 123.0° Si RiDi Ndj νdj *1 46.3758 1.0100 1.58313 59.38 *2 3.3668 2.4940 *3 −14.44732.1850 1.80610 40.93 *4 −9.4876 1.5900 5 (St) ∞ 0.2500 6 8.9451 0.80001.92286 18.90 7 6.8588 1.9450 *8 9.4375 2.3510 1.61881 63.85 *9 −7.12400.1550 *10 7.2603 3.5270 1.61881 63.85 *11 −5.7164 0.5800 12 −4.34441.0300 1.92286 18.90 13 −29.1760 2.9218

TABLE 14 Example 7 Surface Number 1 2 3 4 KA  1.0327202E+00 9.8019961E−01  4.9694277E+00 −2.9099924E+00  A4 −5.9233330E−05−2.8689402E−04 −2.2924366E−05 −1.3621110E−04  A6  1.6622778E−06 2.1692241E−05 −1.4724490E−04 3.5068758E−05 A8  1.0397916E−07−2.6848899E−06  3.3461636E−05 7.3135983E−06 A10  2.7050247E−10−1.0428372E−06 −2.5150332E−06 −2.1791514E−06  A12 −3.6932844E−11−2.4352323E−08 −4.6174102E−08 1.9558743E−07 A14 −2.2402612E−12 1.2497274E−08  1.9894415E−08 2.1777333E−08 Surface Number 8 9 10 11 KA−2.3612553E+00 −6.6531916E−02  4.1053430E−01 9.6877644E−01 A4 3.4471265E−04 −1.0428498E−04 −4.2462103E−05 1.7926632E−05 A6−9.7181061E−05 −5.3405254E−05 −4.4621273E−06 1.3281746E−05 A8−2.5002782E−06  1.1306410E−07  7.9091110E−07 6.4964412E−07 A10−1.5481362E−06 −8.0820586E−07  2.0366571E−08 −4.0400932E−08  A12 8.3508545E−09  1.6002736E−09  2.4018607E−08 5.8714236E−09 A14−1.4760971E−08 −9.9924589E−10 −5.6182023E−09 −5.5298781E−09 

Example 8

FIG. 9 is a cross sectional diagram that illustrates the lensconfiguration of the imaging lens of Example 8. Basic lens data areshown in Table 15 and aspherical surface coefficients are shown in Table16 for the imaging lens of Example 8. In addition, FIG. 18 and FIG. 27are collections of diagrams that illustrate various aberrations of theimaging lens of Example 8 in a state focused on an object at infinity.

TABLE 15 Example 8 f = 3.33, Bf = 3.24, F No. = 2.28, 2ω = 123.2° Si RiDi Ndj νdj *1 46.3736 1.0100 1.58313 59.38 *2 3.3334 2.4570 *3 −14.45861.9610 1.80610 40.93 *4 −9.7697 1.5900 5 (St) ∞ 0.2500 6 9.3810 0.80001.92286 18.90 7 7.0625 2.1580 *8 9.0419 2.3690 1.61881 63.85 *9 −7.04010.1550 *10 7.1408 3.5260 1.58913 61.13 *11 −5.4447 0.5150 12 −4.29950.8180 1.92286 18.90 13 −26.6030 3.2364

TABLE 16 Example 8 Surface Number 1 2 3 4 KA  1.0334726E+00 9.8030124E−01  4.9801959E+00 −2.9122855E+00  A4 −5.8024852E−05−2.8189771E−04 −2.4590119E−05 −1.3544314E−04  A6  1.6956276E−06 2.1923822E−05 −1.4721080E−04 3.5104720E−05 A8  1.0430474E−07−2.7579193E−06  3.3457329E−05 7.3387160E−06 A10  2.4946414E−10−1.0524835E−06 −2.5235853E−06 −2.1960366E−06  A12 −3.8427086E−11−2.4352323E−08 −4.8215408E−08 1.9110873E−07 A14 −2.2861582E−12 1.2203478E−08  1.9791472E−08 2.1131665E−08 Surface Number 8 9 10 11 KA−2.3562538E+00 −6.6647527E−02  4.1052883E−01 9.6875745E−01 A4 3.4502806E−04 −1.0417222E−04 −4.2400364E−05 1.7945755E−05 A6−9.7141826E−05 −5.3439129E−05 −4.4416486E−06 1.3280570E−05 A8−2.5159409E−06  1.1094541E−07  7.9193048E−07 6.4989595E−07 A10−1.5338407E−06 −8.0812181E−07  2.0221549E−08 −4.0389780E−08  A12 1.0116120E−08  1.3572568E−09  2.4127158E−08 5.8406600E−09 A14−1.5851986E−08 −1.0649370E−09 −5.7014824E−09 −5.4950473E−09 

Example 9

FIG. 10 is a cross sectional diagram that illustrates the lensconfiguration of the imaging lens of Example 9. Basic lens data areshown in Table 17 and aspherical surface coefficients are shown in Table18 for the imaging lens of Example 9. In addition, FIG. 19 and FIG. 28are collections of diagrams that illustrate various aberrations of theimaging lens of Example 9 in a state focused on an object at infinity.

TABLE 17 Example 9 f = 3.33, Bf = 3.24, F No. = 2.28, 2ω = 123.0° Si RiDi Ndj νdj *1 46.3736 1.0100 1.58313 59.38 *2 3.3285 2.4450 *3 −14.59701.9320 1.80610 40.93 *4 −9.9257 1.5900 5 (St) ∞ 0.2500 6 9.4702 0.80001.92286 18.90 7 7.1652 2.1650 *8 8.8618 2.3850 1.60300 65.44 *9 −6.98660.1550 *10 7.0553 3.5560 1.58913 61.13 *11 −5.4694 0.5290 12 −4.29520.8000 1.92286 18.90 13 −25.5142 3.2368

TABLE 18 Example 9 Surface Number 1 2 3 4 KA  1.0334431E+00 9.8030077E−01  4.9803975E+00 −2.9122859E+00  A4 −5.8024774E−05−2.8189727E−04 −2.4592151E−05 −1.3541150E−04  A6  1.6955864E−06 2.1923972E−05 −1.4721083E−04 3.5104654E−05 A8  1.0431490E−07−2.7590165E−06  3.3457360E−05 7.3374649E−06 A10  2.5067838E−10−1.0530540E−06 −2.5216200E−06 −2.1893681E−06  A12 −3.8448124E−11−2.4352323E−08 −4.7567233E−08 1.9800451E−07 A14 −2.2859516E−12 1.2838233E−08  2.0615387E−08 2.1789265E−08 Surface Number 8 9 10 11 KA−2.3566731E+00 −6.6641328E−02  4.1054108E−01 9.6875465E−01 A4 3.4500517E−04 −1.0417181E−04 −4.2399135E−05 1.7945446E−05 A6−9.7141907E−05 −5.3439221E−05 −4.4417478E−06 1.3280435E−05 A8−2.5227471E−06  1.1083583E−07  7.9178890E−07 6.4981907E−07 A10−1.5434752E−06 −8.0806789E−07  2.0223586E−08 −4.0474813E−08  A12 1.2915844E−08  1.5164494E−09  2.4212796E−08 5.9003760E−09 A14−1.6042183E−08 −1.0535330E−09 −5.6950966E−09 −5.4939693E−09 

Table 19 shows the positions and the diameters of the openings of thefirst light shielding member 4 and the second light shielding member 5for Examples 1 through 9. The positions are shown such that thedirection toward the image side from reference surfaces is positive. Theunits of the numerical values shown in Table 19 are mm.

TABLE 19 First Light Second Light Shielding Member Shielding MemberDistance from Distance from surface toward surface toward image side ofDiameter of image side of Diameter of second lens opening third lensopening Example 1 1.19 φ3.1 1.45 φ3.6 Example 2 0.97 φ3.1 1.55 φ3.8Example 3 1.06 φ3.1 1.81 φ3.8 Example 4 1.38 φ3.1 2.00 φ3.8 Example 51.00 φ3.1 1.65 φ3.8 Example 6 1.19 φ3.1 2.26 φ4.0 Example 7 1.19 φ3.11.89 φ3.64 Example 8 1.19 φ3.1 2.10 φ3.7 Example 9 1.19 φ3.1 2.11 φ3.8

Table 20 shows the focal length f of the entire lens system, the focallengths f1 through f6 of the first lens L1 through the sixth lens L6,values related to the conditional formulae, and values corresponding toConditional Formulae (1), (2), (2-1), and (3) through (8) for Examples 1through 9. The numbers (1), (2), (2-1), and (3) through (8) in theleftmost column of Table 20 are the numbers of the Conditional Formulae.The numerical values shown in Table 20 are those with reference to the dline except for those in the column related to Conditional Formula (8).The values of dN/dT (L4) and dN/dT (L5) in Table 20 respectively are therelative temperature coefficients of the refractive indices of thematerials of the fourth lens L4 and the fifth lens L5 with respect to awavelength of 632.8 nm within a temperature range from 20° C. to 40° C.Numerical values are shown only for materials of which the relativetemperature coefficients are negative. The units of numerical values fordN/dT (L4) and dN/dT (L5) in Table 20 are −10⁻⁶/° C. The material isshown before the slash within the parentheses, and the manufacturer ofthe material is shown after the slash. Note that in Table 20, K. K.Ohara is shown as OHARA, and HOYA K. K. is shown as HOYA.

TABLE 20 Example 1 Example 2 Example 3 Example 4 Example 5 Example 6Example 7 Example 8 Example 9 f 3.3592 3.3499 3.3117 3.3790 3.34343.3278 3.3052 3.3272 3.3298 f1 −6.3304 −5.9219 −6.0124 −4.9104 −4.9776−6.1887 −6.2800 −6.2129 −6.2030 f2 22.3397 20.8310 25.2380 12.748019.1366 31.3385 28.6511 31.4936 32.4806 f3 −22.1027 −21.5207 −23.9853−28.2556 −20.3131 −30.4341 −39.0517 −37.1106 −38.2754 f4 5.9148 5.79856.0557 7.6865 6.2984 6.2562 6.9368 6.7782 6.8674 f5 5.6010 5.8509 5.75445.1735 5.6496 6.6635 5.7677 5.8515 5.8449 f6 −5.4705 −5.6415 −5.8124−5.8642 −6.0381 −5.9115 −5.6435 −5.6566 −5.6995 f12 −13.5528 −12.8912−10.4902 −14.2720 −9.3149 −9.6789 −10.5949 −9.7580 −9.5665 f45 3.50243.4947 3.5946 3.5743 3.5865 3.9151 3.8001 3.8170 3.8399 (1) f12/f−4.0345 −3.8483 −3.1677 −4.2238 −2.7861 −2.9085 −3.2055 −2.9328 −2.8730(2) |R3/f| 3.5342 4.0140 4.8938 263.9823 5.9140 4.3874 4.3711 4.34564.3838 (2-1) R3/f −3.5342 −4.0140 −4.8938 −263.9823 −5.9140 −4.3874−4.3711 −4.3456 −4.3838 (3) f1/f −1.8845 −1.7678 −1.8155 −1.4532 −1.4888−1.8597 −1.9000 −1.8673 −1.8629 (4) R4/f −2.3295 −2.4140 −2.8645 −3.0094−2.7073 −2.9419 −2.8705 −2.9363 −2.9809 (5) f45/f 1.0426 1.0432 1.08541.0578 1.0727 1.1765 1.1497 1.1472 1.1532 (6) f4/f 1.7608 1.7309 1.82862.2748 1.8838 1.8800 2.0987 2.0372 2.0624 (7) f5/f 1.6674 1.7466 1.73761.5311 1.6898 2.0024 1.7450 1.7587 1.7553 (8) dN/dT(L4) −3.0 −3.0 −2.6(M-PCD4/ (M-PCD4/ (S-PHM53/ HOYA) HOYA) OHARA) (8) dN/dT(L5) −3.0 −3.0−3.0 −3.0 −6.2 −3.0 (M-PCD4/ (M-PCD4/ (M-PCD4/ (M-PCD4/ (S-FPL51/(M-PCD4/ HOYA) HOYA) HOYA) HOYA) OHARA) HOYA)

As can be understood from the above data, the imaging lenses of Examples1 through 9 have six lenses, are configured to be compact, achieve wideangles of view with maximum angles of view within a range from 120° to130°, have small F numbers within a range from 2.2 to 2.3, and favorablycorrect various aberrations to achieve high optical performance.

FIG. 29 illustrates the manner in which imaging apparatuses equippedwith the imaging lens of the present embodiment are mounted on anautomobile 100 as an example of utilization. In FIG. 29, the automobile100 is equipped with an externally mounted camera 101 for imaging ablind spot range at the side surface on the side of the passenger seat,an externally mounted camera 102 for imaging a blind spot range at therear side of the automobile 100, and a internally mounted camera 103which is mounted on the back surface of the rear view mirror and imagesthe same range as the field of view of a driver. The externally mountedcamera 101, the externally mounted camera 102, and the internallymounted camera 103 are imaging apparatuses, and are each equipped withan imaging lens according to an embodiment of the present disclosure andan imaging element that converts optical images formed by the imaginglens into electric signals. The vehicle mounted cameras of the presentembodiment (the externally mounted camera 101, the externally mountedcamera 102, and the internally mounted camera 103) are equipped withimaging lenses according to the embodiment of the present disclosure.Therefore, the vehicle mounted cameras are capable of performing imagingunder low light conditions, have wide angles of view, and can obtainfavorable images from the central portion through the peripheralportions of the image formation regions thereof.

The present disclosure has been described with reference to theembodiments and Examples. However, the present disclosure is not limitedto the above embodiments and Examples, and various modifications arepossible. For example, the values of the radii of curvature, the surfacedistances, the refractive indices, the Abbe's numbers, the asphericalsurface coefficients, etc. of each of the lenses are not limited tothose exemplified in the above Examples, and may be different values.

In addition, materials that satisfy Conditional Formula (8) and areutilizable as optical materials are not limited to the three types shownin the Examples, and performance can be optimized by employing S-PHM52or S-FPM2 by Ohara, FCD1 by HOYA, H-ZPK2 by CDGM Glass, etc., forexample. In addition, M-PCD4 is an optical glass for glass molds byHOYA, but optical glass PCD4 for polishing by HOYA may also be employedto obtain equivalent advantageous effects.

In addition, the imaging apparatus according to embodiments of thepresent disclosure are not limited to vehicle mounted cameras. Theimaging apparatus of the present disclosure may be a camera for aportable terminal, a surveillance camera, a digital camera, etc.

What is claimed is:
 1. An imaging lens consisting of, in order from theobject side to the image side: a first lens having a negative refractivepower and a concave surface toward the image side; a second lens havinga positive refractive power and a convex surface toward the image side;a third lens having a negative refractive power and a concave surfacetoward the image side; a fourth lens having a positive refractive powerand is of a biconvex shape; a fifth lens having a positive refractivepower and is of a biconvex shape; and a sixth lens having a negativerefractive power and a concave surface toward the object side; andConditional Formula (1) below being satisfied:−5<f12/f<−2  (1) wherein f12 is the combined focal length of the firstlens and the second lens, and f is the focal length of the entire lenssystem.
 2. An imaging lens as defined in claim 1, in which ConditionalFormula (1-1) below is satisfied:−4.7<f12/f<−2.3  (1-1).
 3. An imaging lens as defined in claim 1, inwhich Conditional Formula (2) below is satisfied:2<|R3|/f  (2) wherein R3 is the radius of curvature of the surface ofthe second lens toward the object side.
 4. An imaging lens as defined inclaim 3, in which Conditional Formula (2-1) below is satisfied:−300<R3/f<−2  (2-1).
 5. An imaging lens as defined in claim 1, in whichConditional Formula (3) below is satisfied:−2.1<f1/f<−1.3  (3) wherein f1 is the focal length of the first lens. 6.An imaging lens as defined in claim 5, in which Conditional Formula(3-1) below is satisfied:−2.0<f1/f<−1.4  (3-1).
 7. An imaging lens as defined in claim 1, inwhich Conditional Formula (4) below is satisfied:−3.5<R4/f<−2.0  (4) wherein R4 is the radius of curvature of the surfaceof the second lens toward the image side.
 8. An imaging lens as definedin claim 7, in which Conditional Formula (4-1) below is satisfied:−3.2<R4/f<−2.2  (4-1).
 9. An imaging lens as defined in claim 1, inwhich Conditional Formula (5) below is satisfied:0.9<f45/f<1.3  (5) wherein f45 is the combined focal length of thefourth lens and the fifth lens.
 10. An imaging lens as defined in claim9, in which Conditional Formula (5-1) below is satisfied:0.9<f45/f<1.2  (5-1).
 11. An imaging lens as defined in claim 9, inwhich Conditional Formula (6) below is satisfied:1.5<f4/f<3.0  (6) wherein f4 is the focal length of the fourth lens. 12.An imaging lens as defined in claim 11, in which Conditional Formula(6-1) below is satisfied:1.6<f4/f<2.6  (6-1).
 13. An imaging lens as defined in claim 9, in whichConditional Formula (7) below is satisfied:1.4<f5/f<2.2  (7) wherein f5 is the focal length of the fifth lens. 14.An imaging lens as defined in claim 13, in which Conditional Formula(7-1) below is satisfied:1.45<f5/f<2.1  (7-1).
 15. An imaging lens as defined in claim 1, inwhich the material of at least one of the fourth lens and the fifth lenssatisfies Conditional Formula (8) below:dN/dT<0  (8), wherein dN/dT is the relative temperature coefficient ofthe refractive index of the material with respect to a wavelength of632.8 nm within a temperature range from 20° C. to 40° C.
 16. An imagingapparatus equipped with an imaging lens as defined in claim 1.